Method of measuring thickness of cell gap of reflective type liquid crystal display

ABSTRACT

A method of measuring the thickness of a cell gap of a reflective type liquid crystal display. An optical system having a rotating table, an input polarizer, a beam splitter, and a output polarizer is used. A reflective type liquid crystal device is disposed on a rotating table. An incident light is reflected by the liquid crystal device. The reflective type liquid crystal device is located between the input polarizer and the output polarizer. A beta angle β is defined as the angle between the input light polarization and the front liquid crystal director. A first formula is used to express the relationship between the reflectivity R ⊥  and β. The reflectivity is R ⊥  then differentiated by β to obtain a second formula that express the relationship between β max  and the thickness of the cell gap. The rotating table is rotated to measure the maximum value β max  of the angle β. The thickness d can thus be obtained more precisely.

CROSS-REFERENCE TO RELATED APPLICATION

[0001] This application claims the priority benefit of Taiwan application serial no. 89106779, filed Apr. 12, 2000.

BACKGROUND OF THE INVENTION

[0002] 1. Field of the Invention

[0003] The invention relates in general to a method of measuring the thickness of a cell gap of a reflective type liquid crystal display (LCD). More particularly, the invention relates to a method of measuring a thickness of a cell gap of a reflective type mixed-mode twisted nematic (MTN) liquid crystal display.

[0004] 2. Description of the Related Art

[0005] In the recent years, the liquid crystal display, being supported with the development of relative electronic devices, becomes very widely applied with versatile functions. Consequently, the fabrication of liquid crystal displays becomes more complex. Generally speaking, the liquid crystal display can be categorized into reflective type liquid crystal display, transmissive type liquid crystal display and transflective type liquid crystal display.

[0006] In the liquid crystal display, the cell gap is a very important factor to control the characteristics such as brightness, contrast or color. In the current technique for fabricating the liquid crystal display, only the transmissive type liquid crystal display has a measuring method to precisely measure the thickness of the cell gap. This method cannot be applied to the reflective type or transflective type liquid crystal display. If one applies this method to measure the cell gap of the reflective type liquid crystal display, the surface reflection may seriously interfere the correctness of the measurement of the cell gap.

SUMMARY OF THE INVENTION

[0007] The invention provides a method of measuring a cell gap of a reflective type liquid crystal display. In addition to precisely measure the thickness of the cell gap, the methods can also eliminate effect induced from the surface reflection of the reflective type liquid crystal display.

[0008] A relationship between the maximum value β_(max) of a beta angle β and a thickness of the cell gap is derived to calculate the thickness of the cell gap in this method.

[0009] In the method provided by the invention, an optical system is provided. The optical system comprises a light source, a rotating table, an input polarizer, a beam splitter, a output polarizer and a photodiode. The light source includes a He/Ne laser to produce a light beam incident to the input polarizer. A reflective type liquid crystal display device, for example, a reflective type mixed-mode twisted nematic (MTN) is disposed on the rotating table. The reflective type liquid crystall display device comprises a front liquid crystal director and a rear liquid crystal director. The front liquid crystal director indicates the liquid crystal director at the surface of the reflective type liquid crystal display near the beam splitter. The input polarizer is used to receive and polarize the light beam incident from the light source. The beam splitter receives the light coming from the input polarizer. Two light beams are obtained and output by the beam splitter. One light beam is incident back to the reflective type liquid crystal display and reflected thereby. The output polarizer is used to receive the light beam reflected by the liquid crystal display. Along the optical path, the input polarizer and the output polarizer are located at two sides of the reflective type liquid crystal display. The transmissive axis of the input polarizer is perpendicular to the transmissive axis of the output polarizer. The photodiode is used to receive the light beam from the output polarizer to convert the light beam into an electric current signal.

[0010] A beta angle β is defined as the angle between the input polarizer and the front liquid crystal director. A formula as follow is provided: ${X = \sqrt{\varphi^{2} + \left( {\Gamma/2} \right)^{2}}},$

[0011] wherein

Γ=2πdΔn/λ, ${\frac{R_{\bot}}{\beta} = {\left. 0\Rightarrow\beta_{\max} \right. = \frac{\tan^{- 1}\left( {- \frac{X}{\varphi \quad t\quad \tan \quad X}} \right)}{2}}},$

[0012] d is the thickness of the cell gap, λ is about 632.8 nm, Δn is the birefringence (about 0.064), φ is the twisted angle of the liquid crystal, that is, the angle between the front and back liquid crystal directors, about 80° to 90°.

[0013] The reflectivity R_(⊥) is differentiated by the beta angle β to obtain a formula: ${R_{\bot} = {\left( {\Gamma \quad \frac{\sin \quad X}{X}} \right)^{2}\quad \left( {{\sin \quad 2\quad \beta \quad \cos \quad X} - {\frac{\varphi}{X}\cos \quad 2\quad \beta \quad \sin \quad X}} \right)^{2}}},$

[0014] wherein β_(max) is a function of d, Δ, φ, and λ.

[0015] According to the second formula, with constant Δ, φ, λ, β_(max) is only the function of the thickness of cell gap d. The rotating table is then rotated to measure the maximum value of the beta angle β_(max), so that the thickness of the cell gap d can be derived.

[0016] Both the foregoing general description and the following detailed description are exemplary and explanatory only and are not restrictive of the invention, as claimed.

BRIEF DESCRIPTION OF THE DRAWINGS

[0017]FIG. 1 is an optical path design for measuring a cell gap of a reflective type liquid crystal display according to the invention;

[0018]FIG. 2A shows the front and rear liquid crystal directors of the optical path design;

[0019]FIG. 2B show the relationship of various angles between the input polarizer and the output polarizer;

[0020]FIG. 3A shows a relationship between the reflectivity R_(⊥) and the beta angle β; and

[0021]FIG. 3B shows the relationship between β_(max) and the thickness of the cell gap.

DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0022] In FIG. 1, an optical path design of the measurement of a cell gap of a reflective type liquid crystal display is according to the invention is illustrated. An optical system 100 comprising light source 102, a rotating table 104, an input polarizer 106, a beam splitter 108, an output polarizer 110, and a silicon photodiode 112 is provided. The light source 102 includes, for example, a He—Ne laser to produce an incident light beam. A reflective type liquid crystal display 114 is disposed on the rotating table 104. The reflective type liquid crystal display 114 includes a mixed-mode twisted nematic (MTN) liquid crystal display, for example. The reflective type liquid crystal display 114 has a front liquid crystal director and a back liquid crystal director. The front liquid crystal director indicates the liquid crystal director at the surface of the liquid crystal display near the beam splitter 108, while the back liquid crystal director indicates the liquid crystal display at the surface far away from the beam splitter 108.

[0023] The input polarizer 106 receives the light beam incident from the light source 102 polarizes the light beam. The light beam through the beam splitter 108 is then received and split by the splitter 108 into two light beams. One of the light beams is incident on the reflective type liquid crystal display 114, and is reflected thereby. The output polarizer 110 receives the light beam reflected from the liquid crystal display 114 and transmitting through the beam splitter 108. Along the optical path of this light beam, the input polarizer 106 and the output polarizer 110 are at two sides to provide the function of a crossed polarizer. That is, when the transmission axis of the input polarizer 106 is perpendicular to the transmission axis of the output polarizer 110, the reflection from the reflective type liquid crystal display 114 is eliminated. The photodiode 112 is used to receive the light beam transmitting through the output polarizer 110 and to convert the light beam into an electric current signal.

[0024] A beta angle, β, is defined as the angle between the incident polarizer director P_(in) and the front liquid crystal director L_(front). In FIG. 2A, the incident light beam travels through the incident polarizer 200 first, and then travels to the beam splitter 202 to be split into two light beams. One of the light beam is directed to the reflective type liquid crystal display 204 to be reflected thereby. The reflected light beam is then incident to the output polarizer 206. The reflective liquid crystal display 204 further comprises a reflecting mirror 208 on the back surface thereof The front liquid crystal director L_(front) means the liquid crystal director along the surface near the beam splitter 202, while the back liquid crystal director L_(back) means the liquid crystal director along the surface far away from the beam splitter.

[0025] The invention further provides a first formula to express the relationship between the reflectivity R_(⊥) and the beta angle β; ${X = \sqrt{\varphi^{2} + \left( {\Gamma/2} \right)^{2}}};$

[0026] wherein,

Γ=2πdΔ/λ ${\frac{R_{\bot}}{\beta} = {\left. 0\Rightarrow\beta_{\max} \right. = \frac{\tan^{- 1}\left( {- \frac{X}{\varphi \quad t\quad \tan \quad X}} \right)}{2}}},$

[0027] d is the thickness of the cell gap;

[0028] λ is the wavelength of the light source;

[0029] Δn is the birefringence of the liquid crystal; and

[0030] φ is the twisted angle of the liquid crystal, that is, the angle between the front and back liquid crystal directors.

[0031] The definitions of the beta angle β and the twisted angle φ are clearly depicted in FIG. 2B. The longitudinal axis represents the direction of the transmissive axis P_(in) of the input polarizer, and the horizontal axis represents the direction of the transmissive axis P_(out) of the output polarizer. The front liquid crystal director L_(front) and the back liquid crystal director L_(back) intersect each other at the intersection of the longitudinal and horizontal axes. The beta angle β can thus be defined as the angle between the input polarization director P_(in) and the front liquid crystal director L_(front), while twisted angle φ is defined as the angle between the front and rear liquid directors L_(front) and L_(back).

[0032] The reflectivity R_(⊥) is differentiated by the beta angle β to obtain a second formula: ${R_{\bot} = {\left( {\Gamma \quad \frac{\sin \quad X}{X}} \right)^{2}\quad \left( {{\sin \quad 2\quad \beta \quad \cos \quad X} - {\frac{\varphi}{X}\cos \quad 2\quad \beta \quad \sin \quad X}} \right)^{2}}},$

[0033] wherein β_(max) is a function of d, Δn, φ, and λ.

[0034] According to the second formula, provided that d, Δn, φ are constant, β_(max) is only dependent on the thickness of the cell gap d. For example, when the Δn is fixed at about 0.064, φ is fixed between 80° to 90°, and λ is fixed at about 632.8 nm, the thickness of the cell gap d can be obtained from the relationship between d and β_(max) as shown in FIG. 3B. It is clear that thickness of the cell gap d is proportional to β_(max.) The linear curve I represents the relationship when the twisted angle φ is 80°, and the linear curve illustrates the relationship when the twisted angle φ is 90°.

[0035] By substituting the above fixed values of Δn=0.064, φ=80°-90°, and λ=632.8 nm and the measurement of β_(max) into the second formula, the thickness d of the cell gap can be obtained. In the method for measuring the thickness of cell gap d, the magnitude of the light reflected from the liquid crystal display varies when the liquid crystal display is turned. The maximum of the beta angle β can thus be obtained when the maximum reflected light is obtained. Table 1 shows an experimental result of the invention. TABLE Item Twisted angle φ Spacer (μm) β_(max) Thickness d 1 80° 4.25 12 4 2 80° 4.75 16.5 4.5 3 90° 4.24 16 4

[0036] The invention has at least the following advantages:

[0037] (1) The effect of reflection from the reflective type liquid crystal can be eliminated, so that the accuracy of the thickness dis not affected thereby. In the optical system 100, the reflective type liquid crystal display 114 is disposed between the input polarizer 106 and the output polarizer 110. Therefore, as the transmissive axes of the input and output polarizers are perpendicular to each other, the surface reflection is blocked between these two polarizers to eliminate the reflection effect.

[0038] (2) The beta angle β is defined as the angle between the incident polarizer director P_(in), and the front liquid crystal L_(front). According to the required intensity of the light beam, the beta angle β is adjusted. In the normal condition, the beta angle β is adjusted to a non-zero value. When the reflected light has a maximum value, the beta angle β has its maximum value β_(max).

[0039] (3) The maximum value of the beta angle β_(max) is proportional to the thickness of the cell gap d. According to the second formula, an accurate value of the thickness of cell gap d can be derived.

[0040] (4) The first formula provided by the invention can be used as a double check for the derived value of d. As shown in FIG. 3A, each curve showing the relationship between the reflectivity R_(⊥) and the beta angle β represents one different thickness d. For example, the curve a represents a thickness d of 3 μm, curve b is for d=4.5 μm, and curve c is for d=6 μm. The empirical method is to observe the position of the curve. When the curve is shifted (towards left or right for decrease or increase of d, respectively), the thickness d is changed.

[0041] Other embodiments of the invention will appear to those skilled in the art from consideration of the specification and practice of the invention disclosed herein. It is intended that the specification and examples to be considered as exemplary only, with a true scope and spirit of the invention being indicated by the following claims. 

What is claimed is:
 1. A method of measuring a thickness of a cell gap in a reflective type liquid crystal display, comprising: providing a light source to produce a light beam incident onto an optical system, wherein the optical system comprising: a rotating table, on which a reflective type liquid crystal display is disposed, the reflective type liquid crystal display comprising a front liquid crystal director and a back liquid crystal director; an incident polarizer, to receive the light beam incident from the light source, and to polarize the light beam; a beam splitter, to receive the light beam polarized by the incident polarizer and to split the light beam coming from the incident polarizer into two split light beams, wherein one of the split beams is incident onto the reflective type liquid crystal display and reflected thereby; an output polarizer, to receive and polarize the light beam reflected by the reflective type liquid crystal display, wherein the input and output polarizers are located at two sides of an optical path of the reflective liquid crystal display; and a photodiode, to receive the light beam transmitting through the output polarizer, and to convert the light beam into an electric current signal; defining a beta angle as an angle between the incident polarizer and the front liquid crystal director; obtaining a formula between a reflectivity R_(⊥) and a beta angle β as: ${R_{\bot} = {\left( {\Gamma \quad \frac{\sin \quad X}{X}} \right)^{2}\quad \left( {{\sin \quad 2\quad \beta \quad \cos \quad X} - {\frac{\varphi}{X}\cos \quad 2\quad \beta \quad \sin \quad X}} \right)^{2}}},\quad {wherein}$ ${\Gamma = {2\quad \pi \quad d\quad \Delta \quad {n/\lambda}}},{X = \sqrt{\varphi^{2} + \left( {\Gamma/2} \right)^{2}}},$

d is a thickness of a cell gap of the reflective Δn is the birefringence of the liquid crystal, φ is a twisted angle the liquid crystal, and λ is a wavelength of the light source; differentiating the formula of R_(⊥) by the beta angle obtaining a relationship between a reflectivity R_(⊥) and a beta angle β as a second formula: ${\frac{R_{\bot}}{\beta} = {\left. 0\Rightarrow\beta_{\max} \right. = \frac{\tan^{- 1}\left( {- \frac{X}{\varphi \quad t\quad \tan \quad X}} \right)}{2}}},$

wherein β_(max) is a function of d, Δn, φ and λ; turning the rotating table to measure β_(max); and substituting the values of β_(max), Δn, φ and λ into the second formula to derive the value of d.
 2. The method according to claim 1 , wherein the step of providing the light source comprises provides a He/Ne laser.
 3. The method according to claim 1 , wherein the reflective liquid crystal display comprises a mixed-mode twisted nematic liquid crystal display.
 4. The method according to claim 1 , wherein input and output polarizers comprise transmissive axes perpendicular to each other.
 5. The method according to claim 1 , wherein the front liquid crystal director is a liquid crystal director along a surface near the beam splitter.
 6. The method according to claim 1 , wherein the back liquid crystal director is a liquid crystal director along a surface far away from the beam splitter.
 7. The method according to claim 1 , wherein the twisted angle φ is an angle between the front and the back liquid crystal directors.
 8. The method according to claim 1 , wherein the twisted angle φ is about 80° to about 90°.
 9. The method according to claim 1 , wherein Δn is about 0.064.
 10. The method according to claim 1 , wherein λ is about 632.8 nm.
 11. A method for measuring a thickness of cell gap of a reflective type liquid crystal display, comprising: providing the reflective type liquid crystal display, wherein the reflective type liquid crystal display has a front liquid crystal director and a back liquid crystal director; providing an optical system comprising: a rotating table to dispose the reflective type liquid crystal display thereon; an input polarizer to receive and polarize a light beam produced by a light source; a beam splitter to split the light beam polarized by the input polarizer into two split light beams, wherein one of the split light beam is incident onto the reflective type liquid crystal and is reflected thereby; an output polarizer to receive the light beam reflected by the reflective type liquid crystal display, wherein the input and output polarizers are disposed at two sides of the reflective type liquid crystal display; and a photodiode, to receive the light beam from the output polarizer and to convert the light beam into an electric current signal; defining an angle between the front liquid crystal director and the input polarizer as a beta angle β; differentiating a function of reflectivity R_(⊥) of the beta angle β by a factor of a twisted angle φ, wherein the twisted angle φ is the angle between the front and the back liquid crystal directors to obtain a maximum value of the beta angle β_(max), and measuring the value of β_(max) by turning the rotating table; and substituting the measured value of β_(max) to derive the thickness of the cell gap d.
 12. The method according to claim 11 , wherein the light source comprises a He/Ne laser.
 13. The method according to claim 11 , wherein the reflective liquid crystal display comprises a mixed-mode twisted nematic liquid crystal display.
 14. The method according to claim 11 , wherein input and output polarizers comprise transmissive axes perpendicular to each other.
 15. The method according to claim 11 , wherein the front liquid crystal director is a liquid crystal director along a surface near the beam splitter.
 16. The method according to claim 11 , wherein the back liquid crystal director is a liquid crystal director along a surface far away from the beam splitter.
 17. The method according to claim 1 , wherein the function of reflectivity is expressed as: ${R_{\bot} = {\left( {\Gamma \quad \frac{\sin \quad X}{X}} \right)^{2}\quad \left( {{\sin \quad 2\quad \beta \quad \cos \quad X} - {\frac{\varphi}{X}\cos \quad 2\quad \beta \quad \sin \quad X}} \right)^{2}}},$

wherein Γ=2πdΔn/λ, ${X = \sqrt{\varphi^{2} + \left( {\Gamma/2} \right)^{2}}},$

d is the thickness of a cell gap of the reflective Δn is the birefringence of the liquid crystal, φ is the twisted angle the liquid crystal, and λ is the wavelength of the light source
 18. The method according to claim 17 , wherein the twisted angle φ is about 80° to about 90°.
 19. The method according to claim 17 , wherein Δ is about 0.064.
 20. The method according to claim 17 , wherein λ is about 632.8 nm. 